1. 3/23/2015PHY 752 Spring 2015 -- Lecture 231 PHY 752 Solid State Physics 11-11:50 AM MWF Olin 107 Plan for Lecture 23:  Transport phenomena and Fermi liquid theory – Chap. 17 in Marder  Boltzmann equation  Thermoelectric phenomena  Hall effect Contains materials from Marder’s lecture notes

2. 3/23/2015PHY 752 Spring 2015 -- Lecture 232

3. 3/23/2015PHY 752 Spring 2015 -- Lecture 233 Using previous results based on wavepacket of Bloch waves with wavevectors near k c  k and spatially centered at r c  r. Effective Hamitonian with electric and magnetic fields: where Equations of motion

4. 3/23/2015PHY 752 Spring 2015 -- Lecture 234 Equations of motion continued: Marder’s notation for distribution function: Number of electrons in volume density of states

5. 3/23/2015PHY 752 Spring 2015 -- Lecture 235 Properties of the distribution function: Continuity equation: additional term due to particle interactions Boltzmann’s equation:

6. 3/23/2015PHY 752 Spring 2015 -- Lecture 236 Relaxation time approximation to collision term Fermi-Dirac distribution Solution to Boltzmann equation in relaxation time approximation:

7. 3/23/2015PHY 752 Spring 2015 -- Lecture 237 Finding distribution function in relaxation time approximation -- continued Integrating by parts:

8. 3/23/2015PHY 752 Spring 2015 -- Lecture 238 Finding distribution function in relaxation time approximation -- continued

9. 3/23/2015PHY 752 Spring 2015 -- Lecture 239 Finding distribution function in relaxation time approximation -- continued If the relaxation time  E is faster than the other variables, the integral can be approximated as:

10. 3/23/2015PHY 752 Spring 2015 -- Lecture 2310 Application to electrical current in the presence of a uniform electric field

11. 3/23/2015PHY 752 Spring 2015 -- Lecture 2311 Application to electrical current in the presence of a uniform electric field -- continued  Only the Fermi surface contributes to the conductivity

12. 3/23/2015PHY 752 Spring 2015 -- Lecture 2312 Alternate expression: For isotropic system: Application to electrical current in the presence of a uniform electric field -- continued where:

13. 3/23/2015PHY 752 Spring 2015 -- Lecture 2313 Effects of heat and temperature For a constant volume process, the first law of thermo says Define particle current: Define energy current: External force acting on system

14. 3/23/2015PHY 752 Spring 2015 -- Lecture 2314 Effects of heat and temperature – continued Rate of entropy production: Rate of heat production

15. 3/23/2015PHY 752 Spring 2015 -- Lecture 2315 Effects of heat and temperature – continued Heat production per wavenumber and per volume: Connection with Boltzmann distribution in relaxation approximation:

16. 3/23/2015PHY 752 Spring 2015 -- Lecture 2316 Calculation of response coefficients General form of response coeffients:

17. 3/23/2015PHY 752 Spring 2015 -- Lecture 2317 Responses involving thermal and electrical gradients Electrochemical force: Electrochemical flux: Thermal force: Thermal flux:

18. 3/23/2015PHY 752 Spring 2015 -- Lecture 2318 Responses involving thermal and electrical gradients – continued Linear coefficients: Note that these can be calculated from: where

19. 3/23/2015PHY 752 Spring 2015 -- Lecture 2319 Responses involving thermal and electrical gradients – continued Define: Note that:

20. 3/23/2015PHY 752 Spring 2015 -- Lecture 2320 Example: Thermal conductivity Consider the case where there is heat flow but no current:

21. 3/23/2015PHY 752 Spring 2015 -- Lecture 2321 Example: Thermal conductivity -- continued

22. 3/23/2015PHY 752 Spring 2015 -- Lecture 2322 Example: Hall effect

23. 3/23/2015PHY 752 Spring 2015 -- Lecture 2323 Example: Hall effect -- continued

24. 3/23/2015PHY 752 Spring 2015 -- Lecture 2324 Example: Hall effect -- continued

25. 3/23/2015PHY 752 Spring 2015 -- Lecture 2325 Example: Hall effect -- continued

26. 3/23/2015PHY 752 Spring 2015 -- Lecture 2326 Example: Hall effect -- continued where:

27. 3/23/2015PHY 752 Spring 2015 -- Lecture 2327 Example: Hall effect -- continued Hall coefficient: